Investigating the urban air quality effects of cool walls and cool roofs in

May 24, 2019 - Solar reflective cool roofs and walls can be used to mitigate the urban heat island effect. While many past studies have investigated t...
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Investigating the urban air quality effects of cool walls and cool roofs in Southern California Jiachen Zhang, Yun Li, Wei Tao, Junfeng Liu, Ronnen M. Levinson, Arash Mohegh, and George Ban-Weiss Environ. Sci. Technol., Just Accepted Manuscript • DOI: 10.1021/acs.est.9b00626 • Publication Date (Web): 24 May 2019 Downloaded from http://pubs.acs.org on May 25, 2019

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Investigating the urban air quality effects of cool walls and cool roofs in

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Southern California

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Jiachen Zhang1, Yun Li1, Wei Tao2, Junfeng Liu3, Ronnen Levinson4, Arash Mohegh1, George Ban-

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Weiss1,*

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1

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CA 90089, USA

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2 Multiphase

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Mainz, Germany

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3 Laboratory

Department of Civil and Environmental Engineering, University of Southern California, Los Angeles,

Chemistry Department, Max-Planck-Institute for Chemistry, Hahn-Meitner-Weg 1, 55128,

for Earth Surface Processes, College of Urban and Environmental Sciences, Peking

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University, Beijing, 100871, China

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4 Heat

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*Correspondence to George Ban-Weiss, [email protected], 213-740-9124

Island Group, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA

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Abstract

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Solar reflective cool roofs and walls can be used to mitigate the urban heat island effect. While

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many past studies have investigated the climate impacts of adopting cool surfaces, few studies

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have investigated their effects on air pollution, especially on particulate matter (PM). This

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research for the first time investigates the influence of widespread deployment of cool walls on

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urban air pollutant concentrations, and systematically compares cool wall to cool roof effects.

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Simulations using a coupled meteorology-chemistry model (WRF-Chem) for a representative

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summertime period show that cool walls and roofs can reduce urban air temperatures, wind 1 ACS Paragon Plus Environment

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speeds, and planetary boundary heights in the Los Angeles Basin. Consequently, increasing wall

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(roof) albedo by 0.80, an upper bound scenario, leads to maximum daily 8-hour average ozone

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concentration reductions of 0.35 (0.83) ppbv in Los Angeles County. However, cool walls

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(roofs) increase daily average PM2.5 concentrations by 0.62 (0.85) μg m-3. We investigate the

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competing processes driving changes in concentrations of speciated PM2.5. Increases in primary

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PM (elemental carbon and primary organic aerosols) concentrations can be attributed to

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reductions in ventilation of the Los Angeles Basin. Increases in concentrations of semi-volatile

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species (e.g., nitrate) are mainly driven by increases in gas-to-particle conversion due to reduced

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atmospheric temperatures.

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1 Introduction

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Urbanization is occurring at a fast pace around the world; global urban land area in 2030 is

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projected to be up to triple that in 20001. Compared to rural areas with natural land cover, urban

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areas contain more impervious surfaces that are made of solar absorptive and thermally massive

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materials, such as asphalt concrete. Urban areas also contain less vegetation and thus reduced

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evaporative cooling and shade cover. These differences in urban and natural land cover contribute

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to the urban heat island (UHI) effect (i.e., cities being hotter than their surrounding rural areas)2,

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which can, in turn, affect air pollutant concentrations. The air quality effects of urban land

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expansion have been studied in previous research3–7, although only a few studies clearly explained

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the mechanisms driving these effects8–11. Tao et al.8 suggested that with pollutant emissions held

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constant, urbanization in eastern China would increase ozone concentrations from the surface to 4

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km. However, it would also enhance turbulent mixing and vertical advection, therefore reducing

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the concentrations of primary pollutants below 500 m.

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While many studies have explored the air quality impacts of the UHI effect, fewer studies have

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investigated how strategies that mitigate the UHI effect would influence urban air quality12–15. For

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example, adopting solar reflective cool surfaces (roofs, walls, and pavements) increases city albedo

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and the solar radiation reflected by cities, therefore reducing urban surface temperatures and near-

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surface air temperatures16–22. However, adopting cool surfaces might change air quality in

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unexpected ways. For primary pollutants (i.e., pollutants directly emitted to the atmosphere) such

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as elemental carbon (EC), nitric oxide (NO), and carbon monoxide (CO), lower surface

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temperatures in cities may suppress convection and therefore reduce atmospheric mixing heights

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and vertical dispersion of pollutants, leading to increases in pollutant concentrations near the

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ground23. Changes in horizontal temperature distributions can also influence wind speed and

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direction, affecting the horizontal transport and distribution of pollutants. For secondary pollutants

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(i.e., pollutants formed in the atmosphere from primary pollutants), in addition to the previously

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mentioned changes in transport and dispersion of pollutants and their precursors, pollutant

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concentrations can also be influenced by temperature dependent chemical reactions, phase-

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partitioning, and emissions. Tropospheric ozone is primarily formed via reactions between

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nitrogen oxides (NOx) and volatile organic compounds (VOCs). Reductions in dispersion could

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increase both VOC and NOx concentrations, though impacts on ozone could be counterintuitive

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due to non-linearities in ozone chemistry. Lowering air temperature decreases biogenic VOC

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emissions from vegetation, potentially reducing ozone concentrations in urban areas where VOC

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availability limits ozone formation24. Air temperature reduction also slows reactions that produce

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ozone. Therefore, ozone concentrations are expected to decrease with lower temperatures25. 3 ACS Paragon Plus Environment

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Secondary particulate matter includes sulfate, nitrate, ammonium, and secondary organic aerosols

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(SOA). While temperature-dependent reactions that form secondary particulate matter should be

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slower due to reduced temperatures, gas-particle partitioning for semi-volatile species (ammonium

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nitrate and semi-volatile SOA) favors the particle phase26,27. The competing physical and chemical

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processes lead to uncertainties in changes to air pollution concentrations induced by heat island

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mitigation strategies.

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The complexity of the aforementioned processes requires the use of sophisticated models that

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resolve atmospheric physics and chemistry to predict how cool surface adoption would influence

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city-level air quality. Using photochemical models, Taha et al.13,28 estimated that increasing city

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surface albedo would effectively reduce ozone concentrations in Southern California and Central

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California. Epstein et al.23 predicted that 8-hour daily maximum ozone concentrations would

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decrease if cool roofs do not reflect more solar ultraviolet (UV) than do dark roofs; if solar UV

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reflection is increased, ozone concentrations could rise.

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Despite previous literature on the influence of cool roofs on ozone concentrations, there is only

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one study that has investigated the influence of cool roofs on particulate matter23. They found that

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increasing roof albedo would increase the annual mean concentrations of PM2.5, because reduced

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ventilation would suppress dispersion of pollutants. However, they did not investigate (1) the

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various physicochemical processes driving cool roof impacts on PM2.5 concentrations or (2) the

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varying responses of different PM species (e.g., nitrate, sulfate, and organics) to cool roof adoption.

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Cool walls are less studied than cool roofs. Zhang et al.29, for the first time, estimated the influence

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of cool walls on urban climate, and systematically compared the effects of cool walls to cool roofs.

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They found that adopting cool walls in Los Angeles would lead to daily average canyon air

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temperature reductions of up to 0.40 K, which is slightly lower than that induced by adopting cool

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roofs (0.43 K). However, the influence of cool walls on air quality has never been studied.

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To address the aforementioned science knowledge gaps and inform policymaking on heat

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mitigation strategies, we seek to (1) quantify and systematically compare the air quality effects of

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adopting cool walls and roofs, and (2) investigate the physicochemical processes leading to

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changes in particulate matter concentrations.

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2 Method

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2.1 Model description

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We use the Weather Research and Forecasting model coupled with Chemistry Version 3.7 (WRF-

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Chem V3.7), a state-of-the-science climate and air quality model, to estimate the impacts of

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employing cool walls and roofs on air quality30. WRF-Chem has been widely used to study air

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pollution in Southern California11,31,32. Table S2 summarizes our model configuration. The

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following schemes are chosen for WRF physics: the Rapid Radiative Transfer Model (RRTM) for

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long-wave radiation33, the Goddard shortwave radiation scheme34, the Lin et al. scheme35 for cloud

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microphysics, the Grell 3D ensemble cumulus cloud scheme36, and the Yonsei University scheme

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for the planetary boundary layer37.

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Impervious fraction (Figure S3b) and land use classification in urban grid cells (Figure S3c) are

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obtained from the National Land Cover Database (NLCD, 2006)38,39. The Noah land surface

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model40 simulates land-atmosphere interactions in non-urban grid cells and for the pervious

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portion of urban grid cells. The single-layer urban canopy model resolves urban physics and 5 ACS Paragon Plus Environment

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simulates land-atmosphere interactions for the impervious portion of urban grid cells41. Urban grid

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cells are classified as low-intensity residential (“Developed, Open Spaces” and “Developed, Low

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Intensity” in NLCD), high-intensity residential (“Developed, Medium Intensity” in NLCD), and

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commercial/industrial (“Developed, High Intensity” in NLCD). Urban morphology (i.e., roof

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width, canyon floor width, and building height) is determined for each urban land use type based

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on real-world building and street datasets for Los Angeles County, following Zhang et al29; the

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datasets include National Urban Database and Access Portal (NUDAPT)42, the Los Angeles

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Region Imagery Acquisition Consortium (LARIAC)43, and LA County Street and Address File44.

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Since the default WRF-Chem is not compatible with the NLCD land use classification system, we

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modify the model code to allow for use of NLCD urban land use types, following Fallmann et

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al.45. We also implement satellite-based green vegetation fraction into the model following

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Vahmani and Ban-Weiss21.

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Gas phase chemistry is simulated using the Regional Atmospheric Chemistry Mechanism

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(RACM)46 scheme, further updated by National Oceanic and Atmospheric Administration

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(NOAA) Earth System Research Laboratory (ESRL)32. The RACM-ESRL scheme covers organic

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and inorganic chemistry simulating 23 photolysis and 221 other chemical reactions47. The Modal

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Aerosol Dynamics Model for Europe (MADE) simulates aerosol chemistry48. The volatility basis

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set (VBS) is used for simulating secondary organic aerosols49.

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We evaluate modeled ozone and PM2.5 concentrations against observations (Figures S1 and S2,

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Table S1) from the Environmental Protection Agency’s Air Quality System in Section S1 of the

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Supporting Information. Although our model underestimates ozone and PM2.5 concentrations at

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higher concentrations, the bias in baseline concentrations does not necessarily lead to bias in

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estimated changes induced by adopting cool surfaces.

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2.2 Simulation domains

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We simulate three nested domains (d1, d2, and d3, as shown in Figure S3a) with 30 layers in the

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vertical at horizontal resolutions of 18 km, 6 km, and 2 km, respectively. The three domains each

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cover the Southwestern United States (d1); Central and Southern California (d2); and Southern

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California, including Los Angeles and San Diego (d3). Each outer domain provides boundary

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conditions for the adjacent inner domain. In this paper we report results for the innermost domain.

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2.3 Emission inventories

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WRF-Chem requires gridded emissions inputs for each simulation. We use state-of-the-science

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emission inventories from the South Coast Air Quality Management District (SCAQMD) and

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California Air Resources Board (CARB) for the year 2012 (i.e., the most up-to-date inventories as

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of writing this paper). For the outer two domains (d1 and d2), hourly emissions for the entire year

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at 4-km resolution are provided by CARB for California50. Emissions outside California, but

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within the simulation domain, are from National Emissions Inventory (NEI) by the Environmental

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Protection Agency for the year 201151. For the innermost domain (d3), we use hourly emissions

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for the entire year at 4-km resolution provided by SCAQMD52 . These emissions represent all

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anthropogenic sources including motor vehicles; point sources such as refineries; and off-road

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sources, such as construction. Emission inventories are regridded to match the grid for the modeled

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domains and chemical speciation for RACM-ESRL and MADE/VBS mechanisms used in this

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study. The Model of Emissions of Gases and Aerosols from Nature (MEGAN) is used to generate

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temperature-dependent biogenic organic emissions53. Note that anthropogenic emissions are not 7 ACS Paragon Plus Environment

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sensitive to ambient temperatures in our study. Though some anthropogenic emissions may be

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temperature dependent (e.g., evaporative emissions of VOCs from gasoline powered vehicles),

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this effect is not simulated in this study, as anthropogenic emissions are obtained directly from

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input datasets.

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2.4 Simulation design

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To investigate the air quality effects of cool walls and roofs in Southern California, we simulate

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three scenarios: CONTROL, where wall, roof, and pavement albedos are each set to 0.10;

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COOL_WALL, where wall albedo is increased to 0.90; and COOL_ROOF, where roof albedo is

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increased to 0.90. These cool surface albedos are intentionally chosen to quantify the upper bound

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effects of adopting cool surfaces (i.e., increasing surface albedo by 0.80). Note that cool surface

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albedos of actual cool walls and roofs are usually lower than 0.90. For example, the albedo of a

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bright-white cool roof may decrease to 0.60–0.70 from an initial albedo of 0.80–0.90 after several

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years of soiling and weathering54,55. In order to test the linearity of changes in air pollutant

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concentrations to albedo increases, we add two additional scenarios where wall albedo and roof

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albedo are each increased by 0.40.

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Simulations are performed for 28 June 2012 to 11 July 2012, with the first five days discarded as

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model “spin-up” to reduce the possible influence of inaccuracies in input initial conditions on our

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analysis. We analyze the results from 00:00 local standard time (LST) on July 3 to 00:00 LST on

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July 12. Section S3 in the Supporting Information demonstrates that the meteorology during our

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analysis period is representative of summertime meteorology in Southern California. Thus, our

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results are representative of changes induced by adopting cool surfaces under typical summertime 8 ACS Paragon Plus Environment

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conditions in Southern California. The paired Student’s t-test (n = 9 analyzed days) is used to

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assess whether the changes in cool surface scenarios relative to CONTROL are statistically

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distinguishable from zero.

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2.5 Method of attributing the changes in PM to ventilation versus other factors

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Carbon monoxide (CO) is considered a chemically inert pollutant at urban scale, with

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concentrations controlled by meteorological conditions. Therefore, past studies have used CO as

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a tracer for transport and dispersion of pollutants9,56. Similarly, in our study, we use the increase

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in CO concentration relative to CONTROL to quantify the increase in PM2.5 that is attributable to

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ventilation (∆𝐶𝑃𝑀(vent)), as

∆𝐶𝑃𝑀(vent) =

∆𝐶CO 𝐶CO

× 𝐶𝑃𝑀

(1)

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where ∆𝐶CO is the change in CO mixing ratio (ppbv) relative to CONTROL, 𝐶CO is the mixing

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ratio (ppbv) of CO for CONTROL, 𝐶𝑃𝑀 is the concentration (μg m-3) of a PM species (i.e., total

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PM2.5, sulfate, nitrate, elemental carbon, primary organic aerosol, anthropogenic secondary

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organic aerosols, or biogenic secondary organic aerosols) for CONTROL, and all variables are

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spatial averages over urban areas in Los Angeles County.

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The change in concentration of a PM2.5 species that is not attributable to ventilation ∆𝐶𝑃𝑀(no vent)

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(μg m-3) is then calculated as

∆𝐶𝑃𝑀(no vent) = ∆𝐶𝑃𝑀 ―

∆𝐶CO 𝐶CO

× 𝐶𝑃𝑀

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In this way, we attribute increases in PM2.5 species to reductions in ventilation and changes in all

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other processes. Note that while sea salt aerosols contribute to total PM2.5 concentrations, we omit

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this species from the discussion because they are naturally produced and are not a public health

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concern. Reductions in ventilation may also contribute to less vertical mixing and consequent

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reductions in dry deposition of pollutants.

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2.6 Caveats

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In this study, we assume that adopting cool surfaces would not change reflectance in the UV

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spectrum (280–400 nm). However, based on spectral reflectance measurements, UV reflectance

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could increase from adopting cool roofs23. Increases in UV reflectance could enhance ozone

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production and atmospheric oxidation capacity, which influences the formation of other secondary

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pollutants. Therefore, changes in ozone are a result of competing effects among (a) ozone increases

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induced by enhanced UV reflection, (b) ozone decreases induced by decreased temperatures, and

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(c) ozone changes induced by reduced ventilation, which could affect the dispersion of ozone and

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its precursors.

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The influence of adopting cool surfaces is likely to vary by city due to differences in baseline

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climate and land cover (e.g., vegetation distributions, building distributions, urban canyon

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morphology). Also note that results might be different if simulated using another model or using

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different parameterizations. For example, the single layer urban canopy model does not explicitly

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resolve individual buildings.

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Note that the urban morphology is derived using gross wall area (including windows) instead of

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net wall area (excluding windows). In Los Angeles County, citywide ratio of net wall area to gross

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wall area is 83%.29 In reality, windows may not be changed to cool colors. Therefore, a portion of 10 ACS Paragon Plus Environment

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walls may not be able to be made solar reflective and our study may overestimate the influence of

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adopting cool walls.

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3 Results and discussion

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By comparing changes in air pollutant concentrations for increasing albedo by 0.80 versus 0.40

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relative to CONTROL, we find that the changes in air pollutant concentrations are approximately

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linear to surface albedo change (Section S4 in the Supporting Information). Therefore, the results

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reported for albedo increase of 0.80 can be interpolated to other albedo changes. For simplicity,

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we report only results for COOL_WALL and COOL_ROOF in the main body.

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3.1 Meteorological conditions

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Figure 1 shows spatial distributions of near-surface air temperatures in the afternoon and evening.

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(Diurnal cycles of near-surface air temperatures are shown in Figure S4.) For the CONTROL

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scenario (Figure 1a), temperatures in inland areas are hotter than coastal areas, as expected.

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Temperature reductions induced by adopting cool surfaces are higher in inland areas than in coastal

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areas (Figure 1b,c). This is due to an accumulation effect in air temperature reduction as the sea

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breeze advects air from the coast to inland.

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Although total wall area in Los Angeles County is larger than roof area by a factor of 1.7, daily

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average solar irradiance (W m-2) on walls is 38% of that on roofs29. In addition, 50-59% of the

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solar radiation reflected by cool walls is absorbed by opposing walls or pavements, while all the

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radiation reflected by cool roofs escapes the urban canopy in the model29. Therefore, daily average

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temperature reductions induced by cool roofs (0.45 K) are larger than cool walls (0.24 K) over

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urban areas in Los Angeles County, as shown in Table 1. Cool roofs are simulated to induce larger

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temperature reductions than cool walls at both 14:00 LST (daytime) and 20:00 LST (nighttime).

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Note that past studies investigating how air temperatures influence atmospheric chemistry often

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report 2-meter air temperatures (“T2”)8,45. However, 2-meter air temperature is a diagnostic

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variable that is not used in model calculations of atmospheric chemistry. The chemistry model

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actually uses the four-dimensional (x, y, z, t) atmospheric temperature. Therefore, we present

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temperatures in the lowest atmospheric layer as “near-surface air temperature” rather than “T2.”

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Figures S5 and S6 show diurnal cycles and spatial maps of 10-meter horizontal wind speeds, and

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Figure S7 shows horizontal wind vectors. For the CONTROL scenario, winds are southwesterly

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from coast to inland and wind speed is higher during daytime than nighttime. As shown in Table

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1, spatially averaged wind speed in urban areas is 4.2 m s-1 and 2.3 m s-1 at 14:00 LST and 20:00

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LST, respectively. Simulations predict that adopting cool walls (roofs) decreases onshore wind

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speeds by 0.06 (0.21) m s-1 at 14:00 LST and 0.08 (0.09) m s-1 at 20:00 LST. This can be explained

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by the reduced temperature difference between urban land and ocean, which is a driver for the sea

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breeze.

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Figure S8 show the diurnal cycle of planetary boundary layer (PBL) height. PBL height reaches

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its maximum at 12:00 LST. Adopting cool walls reduces PBL height by 3-7% at most times of

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day. Adopting cool roofs reduces PBL height by about 5% at night and about 10% during the day.

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The reduction in PBL height can be attributed to decreases in surface temperatures and consequent

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reductions in convection. Decreases in wind speeds and PBL height tend to reduce ventilation for

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pollutants. The influence of changes in ventilation on particulate matter is discussed in Section

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3.5.1.

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3.2 Spatial distribution of ozone concentrations

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Figure 2 shows the spatial distribution of daily maximum 8-hour average (MDA8) ozone

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concentrations. MDA8 ozone is regulated by the National Ambient Air Quality Standards of the

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Environmental Protection Agency. For the CONTROL scenario, the ozone concentration over

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urban areas is lower than rural areas because (a) southwesterly winds transport ozone and its

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precursors from the coast to the inland areas, creating an accumulation effect as this secondary

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pollutant is generated in the atmosphere; and (b) nitric oxide emissions in urban areas can titrate

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ozone. Adopting cool walls can decrease the spatially averaged MDA8 ozone concentration by

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0.35 ppbv in the urban areas of Los Angeles County (Table 1). These decreases in ozone

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concentrations are likely due to reductions in temperature-dependent ozone formation. Adopting

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cool roofs can lead to a greater reduction in MDA8 ozone concentration (0.83 ppbv) than cool

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walls. This is likely because the near-surface air temperature reductions induced by cool roofs are

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larger than that induced by cool walls during daytime (Figure S4) and thus the decreases in reaction

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rates for ozone production are larger for COOL_ROOF than COOL_WALL relative to CONTROL.

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As mentioned in Section 2.5, we assume that the UV reflectance of cool surfaces is the same as

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dark surfaces. Similarly, Epstein et al23 report reductions in ozone concentrations in most Southern

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California regions due to adopting cool roofs when UV reflectance is assumed to be held constant.

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(Note that they also find that ozone concentrations could increase if the difference in UV

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reflectance between cool and dark roofs follows an upper bound scenario.)

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3.3 Spatial distribution of PM2.5 species

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Figure 3 shows the spatial distribution of daily average PM2.5 species concentrations and changes

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due to adopting cool surfaces. PM2.5 concentrations reported here represent dry particle mass.

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Spatial distributions of PM2.5 species concentrations in the CONTROL scenario are mainly

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attributable to spatial patterns in emissions and meteorology. For example, when the sea breeze

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advects air from the coast to inland, EC, a primary pollutant, accumulates, leading to higher

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concentrations in locations further east. For spatial distributions of sulfate concentrations, there

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are higher concentrations near the ports of Los Angeles and Long Beach that are likely due to hot

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spots in SO2 (the precursor of secondary sulfate) and primary sulfate emissions from ships and

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power plants (Figure S9). Meanwhile, southwesterly winds then transport these emissions to

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downtown Los Angeles, making concentrations downtown greater than those further east. The

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spatial variability of anthropogenic and biogenic SOA is relatively small compared to other species.

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The concentrations of total PM2.5 and each individual species increase due to cool surface adoption

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(Figure 3). The increase in each PM2.5 species induced by adopting cool roofs is larger than that

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induced by cool walls, though their spatial patterns are similar. Spatial distributions of increases

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in total PM2.5 and individual species (except nitrate) are consistent with the spatial patterns of

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absolute concentrations in the CONTROL scenario. In other words, the regions with the highest

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baseline concentrations show the largest changes in PM2.5 due to meteorological shifts from cool

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surface adoption. The exception is for nitrate, which shows larger increases in urban residential

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areas northeast of downtown where baseline concentrations are low, rather than downtown where

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baseline concentrations are the highest in CONTROL. This is likely due to the greater temperature

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reductions in regions northeast of downtown Los Angeles relative to downtown, especially at night

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(Figure 1b,c). The processes leading to nitrate increases will be discussed in Section 3.5. The 14 ACS Paragon Plus Environment

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increase in SOA is relatively smaller than other species, which will also be explained in Section

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3.5.

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3.4 Diurnal cycles of PM2.5 species concentrations

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Figure 4 shows the diurnal cycles of spatially averaged PM2.5 species concentrations and their

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changes in the urban areas of Los Angeles County. For the CONTROL scenario, PM2.5, nitrate,

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ammonium, sulfate, EC, and primary organic aerosol (POA) concentrations reach their maximum

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between 08:00 and 09:00 LST and their minimum at 16:00 LST, while biogenic and anthropogenic

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SOA reach their maximum near 14:00 LST and their minimum at night. The diurnal cycles of

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PM2.5 concentrations can be attributed to the diurnal variation of (1) emissions (Figure S10); (2)

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PBL height (Figure S8a), which peaks at 12:00 LST; (3) wind speed (Figure S5), which peaks at

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14:00 LST; and (4) photochemical reaction rates for secondary species that depend on UV

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radiation and temperature (Figure S4a).

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Raising roof or wall albedo leads to increases in concentrations of total PM2.5 and most individual

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species (except for biogenic SOA) throughout the day (Figure 4). Increases in nitrate

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concentrations are the largest among all PM2.5 species, followed by increases in POA, sulfate, and

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ammonium, while the increases in concentrations of other PM2.5 species are relatively small. The

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changes in speciated PM2.5 concentrations due to adopting cool walls or roofs vary by time of day,

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and the mechanisms contributing to the changes will be discussed in Section 3.5. For all PM2.5

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species except biogenic SOA, increases in PM2.5 concentrations induced by adopting cool roofs

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are larger than those induced by adopting cool walls during most daytime hours (07:00-19:00 LST).

324

On daily average, cool roof adoption contributes to greater increases in particulate matter than cool

325

wall adoption (Table 1) for total PM2.5 and each species. Daily average increases in total PM2.5

326

concentrations are simulated to be 0.62 (0.85) μg m-3 upon increasing wall (roof) albedo by 0.80 15 ACS Paragon Plus Environment

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in July in Los Angeles County. Compared to the national annual and 24-hour PM2.5 standard of 12

328

μg m−3 and 35 μg m−3, respectively, increases in PM2.5 concentrations reported here have the

329

potential for increasing exceedance days of federal air quality standards. The grid cell containing

330

Mira Loma (i.e., the most polluted PM2.5 monitoring station in Southern California) is simulated

331

to have PM2.5 increases of 0.84 (1.05) μg m−3 due to adopting cool walls (roofs) in summer. Epstein

332

et al. (2018) estimate that annual average PM2.5 concentrations at Mira Loma would increase by

333

0.19 μg m-3 due to adopting cool roofs, which they compute would result in an increase of 2/3

334

exceedance day for the 24-hr federal PM2.5 standard. (The number of exceedance days is not an

335

integer because they report 3x3 cell moving averages.) Thus, even though these changes may look

336

small, they have the potential to increase the annual number of days exceeding air quality standards

337

and are therefore important for regulatory agencies in controlling PM2.5 pollution.

338

3.5 Mechanisms that lead to changes in PM2.5 concentrations

339

As mentioned in the introduction, adopting cool surfaces can influence PM2.5 concentrations

340

mainly via (1) reducing ventilation, (2) slowing temperature dependent reactions and emissions,

341

and (3) increasing the likelihood that semi-volatile species will partition to particle phase. In the

342

following sections we report on the relative importance of these pathways.

343

3.5.1 Ventilation

344

For primary pollutants such as elemental carbon (EC), mass concentrations depend highly on

345

ventilation and are insensitive to atmospheric chemistry in the model. (Note that strictly speaking,

346

hydrophilic species can coat EC and increase its hygroscopicity, enabling the in-cloud wet

347

scavenging of EC57. This so-called “aging process” depends on temperature-dependent

348

atmospheric photochemical reactions that form hydrophilic species, such as sulfate. However, the 16 ACS Paragon Plus Environment

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aging of EC should not be a very important process during summer when there is little precipitation

350

in the Los Angeles Basin.) Decreases in ventilation (Section 3.1) impede the dilution and transport

351

of pollutants in source regions and may also reduce dry deposition, leading to increases in near-

352

surface pollutant concentrations. This ventilation effect is driven by vertical and horizontal mixing

353

of pollutants in the planetary boundary layer, which can be investigated using PBL height and

354

surface wind speeds, respectively. Figure 5 shows that fractional increase in EC is positively

355

correlated with the fractional reductions in PBL height and 10-meter wind speed. Fractional

356

reduction in PBL height can explain 42% of the variability in the fractional increase in EC

357

concentrations for both COOL_WALL – CONTROL and COOL_ROOF – CONTROL. Fractional

358

reduction in horizontal wind speed explains 17% (79%) of the variability in fractional increase of

359

EC concentrations due to adopting cool walls (roofs).

360

3.5.2 Quantifying the relative importance of ventilation versus other factors for driving

361

changes in PM

362

Following the method described in Section 2.5, we quantify increases in PM2.5 species that can be

363

attributed to reductions in ventilation and changes in other processes. As indicated in Figure 4,

364

after removing the effects of ventilation, the change in spatially averaged EC and POA is close to

365

zero. Therefore, increases in primary pollutant (EC and POA) concentrations are attributable to

366

suppressed ventilation. A large fraction of the increase in sulfate from cool surface adoption can

367

be attributed to suppressed ventilation. Other driving processes can affect sulfate concentrations:

368

(a) reductions in temperature-dependent reaction rates would decrease sulfate production; and (b)

369

changes in cloud cover can also influence in-cloud SO2 oxidation, which occurs faster than gas-

370

phase oxidation of SO2 if clouds are present. When the ventilation effect is excluded, sulfate

371

concentrations slightly increase from 04:00 to 14:00 LST but decrease at most other hours, due to 17 ACS Paragon Plus Environment

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372

adopting cool surfaces. Nevertheless, ventilation is the dominant process leading to sulfate

373

increases, contributing to 76 % (91%) of the daily average increase for COOL_WALL –

374

CONTROL (COOL_ROOF – CONTROL).

375

On the other hand, the ventilation effect accounts for a small portion of the increase in semi-volatile

376

species such as nitrate and ammonium (in the form of ammonium nitrate). Concentrations of these

377

particulate species rise drastically even when the ventilation effect is excluded. This is because the

378

reaction between gas-phase ammonia and nitric acid that forms particulate nitrate is reversible,

379

and the equilibrium constant for the reaction is highly temperature dependent. Temperature

380

reductions would cause gas to particle conversion and increase the concentrations of ammonium

381

nitrate26. Note that the amount of nitrate at equilibrium has a non-linear relationship with

382

temperature. Thus, the relationship between increase in nitrate concentration due to gas-to-particle

383

conversion (Figure 4) and temperature reduction is not linear; the increase in nitrate depends not

384

only on the magnitude of temperature reduction but also the baseline temperature. In contrast to

385

shifting equilibrium of the reaction between nitric acid and ammonia, which would increase nitrate,

386

cool surfaces adoption may also reduce photochemistry and impede the formation of nitric acid

387

precursors (i.e., OH and NO2) during the day, leading to a reduction in nitrate. Increased gas-to-

388

particle conversion and suppressed ventilation outweigh reductions in photochemistry, leading to

389

overall increases in nitrate concentrations (Figure 4).

390

For secondary organic aerosols (SOA), reductions in ventilation should lead to increases in SOA,

391

while temperature decreases would be expected to cause (a) increases in gas-to-particle conversion

392

for semi-volatile species, which would lead to SOA increases, and (b) reduced rates of

393

temperature-dependent reactions, which would lead to SOA decreases. Biogenic SOA may also

394

be influenced by reductions in temperature dependent VOC emissions (e.g., isoprene) from 18 ACS Paragon Plus Environment

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vegetation (Figure S11). As shown in Figure 4, both anthropogenic and biogenic SOA increase

396

when including the influence of changes in ventilation, but decrease when ventilation changes are

397

excluded. Daily average SOA concentrations increase by 0.018 (0.046) μg m-3 for COOL_WALL

398

(COOL_ROOF) relative to CONTROL. After removing the ventilation effect, daily average SOA

399

concentrations decrease by 0.057 (0.071) μg m-3 for COOL_WALL (COOL_ROOF) relative to

400

CONTROL. This means that SOA reductions induced by slowed temperature dependent reactions

401

and biogenic emissions outweigh the expected increases in semi-volatile SOA species due to phase

402

partitioning. On the other hand, increases in SOA due to suppressed ventilation and increased gas-

403

to-particle conversion outweigh decreases in SOA due to reduced reaction and emission rates.

404

These competing effects lead to an overall increase in SOA concentrations, although fractional

405

increases are small relative to other species.

406

In this paper, we discuss the climate and air quality implications of cool roofs and cool walls,

407

which have been used in cities to reduce temperatures and thus combat global warming and urban

408

heat islands. Our results show that reductions in urban surface temperatures lead to both co-

409

benefits of reduced ozone concentrations and penalties of increased PM2.5 concentrations,

410

potentially changing the exceedance days of federal air quality standard in the Los Angeles Basin.

411

We suggest further studies to assess the air quality effects of other heat strategies and the effects

412

in other cities. For policy makers, it is important to assess the effects of environmental solutions

413

from a systematic perspective, i.e., looking at heat mitigation impacts not just from a climate

414

perspective but also from an air quality perspective.

415

19 ACS Paragon Plus Environment

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Acknowledgements

417

This research was supported by the California Energy Commission under contract EPC-14-010,

418

and the National Science Foundation under grants CBET-1512429 and 1752522. This work was

419

also supported by the Assistant Secretary for Energy Efficiency and Renewable Energy, Building

420

Technologies Office of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.

421

Computation for the work described in this paper was supported by the University of Southern

422

California’s Center for High-Performance Computing (https://hpcc.usc.edu/). We thank Scott

423

Epstein and Sang-Mi Lee at South Coast Air Quality Management District for providing us

424

emission datasets. We also thank Pouya Vahmani, Haley Gilbert, Pablo Rosado, Hugo Destaillats,

425

and Xiaochen Tang at Lawrence Berkeley National Laboratory, Dan Li at Boston University,

426

Ravan Ahmadov and Stu McKeen at National Oceanic and Atmospheric Administration, Joachim

427

Fallmann at Johannes Gutenberg University Mainz, Gert-Jan Steeneveld at Wageningen

428

University, and Jan Kleissl at University of California, San Diego for their helpful suggestions.

429

Supporting Information

430

Model evaluation, description of the simulated period, and further detail on results. This material

431

is available free of charge via the Internet at http://pubs.acs.org.

432

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Table 1. Spatially averaged meteorological variables and pollutant concentrations for the CONTROL scenario, and the change relative to CONTROL for COOL_WALL and COOL_ROOF. Values represent spatial averages in Los Angeles County (shown in Figure S3b) for urban grid cells from 00:00 LST on July 3 to 00:00 LST on July 12. CONTROL

COOL_WALL minus CONTROL

COOL_ROOF minus CONTROL

Daily average near-surface air temperature a (K)

292.85

-0.24

-0.45

10-meter wind speed at 14:00 LST (m s-1)

4.15

-0.06

-0.21

10-meter wind speed at 20:00 LST (m s-1)

2.28

-0.08

-0.09

Daily maximum 8-hour average ozone concentration (ppbv) Daily average PM2.5 concentration (μg m-3)

38.47

-0.35

-0.83

12.25

0.62

0.85

Daily average nitrate concentration b (μg m-3)

0.89

0.11

0.18

Daily average ammonium concentration b (μg m-3)

0.98

0.07

0.10

Daily average sulfate concentration b (μg m-3)

1.91

0.11

0.13

Daily average EC concentration b (μg m-3)

0.87

0.05

0.06

Daily average anthropogenic SOA concentration b (μg m-3)

1.22

0.01

0.04

Daily average biogenic SOA concentration b (μg m-3)

0.51

0.01

0.01

Daily average POA concentration b (μg m-3)

1.90

0.12

0.14

598

a

599 600

b

Near-surface air temperature refers to the temperature in the lowest atmospheric layer.

Mass concentrations for particles with diameter less than 2.5 μm (i.e., nuclei and accumulation mode) are included for each species.

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602

603 604 605 606

Figure 1. Spatially resolved near-surface air temperatures (K) at 14:00 LST and 20:00 LST for (a) the CONTROL scenario, and the difference relative to CONTROL for (b) COOL_WALL and (c) COOL_ROOF. Values are temporally averaged over the period of 00:00 LST on July 3 to 00:00 LST on July 12.

607

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609 610

611 612 613 614 615 616

Figure 2. Spatially resolved daily maximum 8-hour average (MDA8) ozone concentrations (ppbv) for (a) the CONTROL scenario, and changes relative to CONTROL for (b) COOL_WALL and (c) COOL_ROOF. Changes that are not statistically distinguishable from zero (see section 2.4 for details on statistical analysis) in (b) and (c) are dotted. Values are temporally averaged over the period of 00:00 LST on July 3 to 00:00 LST on July 12.

617

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618

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619 620 621 622 623

Figure 3. Daily average PM2.5 concentrations (μg m-3) by species for CONTROL (left column), as well as the differences for COOL_WALL – CONTROL (middle column) and COOL_ROOF – CONTROL (right column). Differences that are not statistically distinguishable from zero (see Section 2.4 for details on statistical analysis) are shaded in gray (middle and right columns of panels). Values are temporally averaged over the period of 00:00 LST on July 3 to 00:00 LST on July 12.

624

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626 627 628 629 630 631

Figure 4. Diurnal cycles of spatially averaged PM2.5 concentrations by species. The left column shows the diurnal cycle of spatially averaged PM2.5 (μg m-3) for CONTROL, COOL_WALL, and COOL_ROOF. The right column shows the differences in PM2.5 species for COOL_WALL – CONTROL and COOL_ROOF – CONTROL and the differences if ventilation effect is excluded. Values represent spatial averages in Los Angeles County (i.e., shown in Figure S3b) for urban grid cells from 00:00 LST on July 3 to 00:00 LST on July 12. Note that vertical axis ranges vary for each species.

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633 634 635 636 637 638 639

Figure 5. Scatter plots showing fractional increase in EC concentrations induced by cool walls and cool roofs versus (a) fractional reduction in PBL height and (b) fractional reduction in 10-meter wind speed. The value on each dot represents the hour of day (e.g., 9 = 09:00 LST). Least-squares linear regressions and corresponding coefficients of determination (R2) are also shown. Values represent spatial averages in Los Angeles County (i.e., shown in Figure S3b) for urban grid cells from 00:00 LST on July 3 to 00:00 LST on July 12.

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